In the quantum scheme, the WDW equation is constructed and analytically solved for various instances given by the same parameter space from the classical study. First in fig. REF  we presented four different examples due to \(\rm Q\)  of the evolution of the probability density \(\rm \rm |\Psi |^{2}\)  in terms of \(\rm V\)  and \(\rm \phi _{2}\) . All cases display the expected damped behavior as \(\rm V\)  and \(\rm \phi _{2}\)  evolve. Remarkably, when \(\rm Q \ll 0\)  the probability density tends to resemble to the isotropic case [1]}. This result might indicate that for a fixed set of parameters, the anisotropies quantum-mechanically vanish for very small values of the parameter \(\rm Q\) . Besides, this upshot (at least for small initial anisotropies) was already reported in [2]}. In the second example (fig. REF ) the probability density also dies away as \(\rm V\)  and \(\rm \phi _{2}\)  evolve. However, this time \(\rm Q\)  compresses the length over the axis on which the scalar field unfolds as time goes by, which in turns delays the progression of the wave function, hence retarding as well the accelerated expansion.
